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98 research outputs found

Scaled momentum distributions for K-S(0) and Λ /̄ Λ in DIS at HERA

Author: Abdullah WATW
Abramowicz H
Abt I
Adamczyk L
Adamus M
Aggarwal R
Antonelli S
Antonioli P
Antonov A
Arneodo M
Aushev V
Aushev Y
Bachynska O
Bamberger A
Barakbaev AN
Barbagli G
Bari G
Barreiro F
Bartosik N
Bartsch D
Basile M
Behnke O
Behr J
Behrens U
Bellagamba L
Bertolin A
Bhadra S
Bindi M
Blohm C
Bokhonov V
Bold T
Bondarenko K
Boos EG
Borras K
Boscherini D
Bot D
Brock I
Brownson E
Bruemmer N
Brugnera R
Bruni A
Bruni G
Brzozowska B
Bussey PJ
Bylsma B
Caldwell A
Capua M
Carlin R
Catterall CD
Chekanov S
Chwastowski J
Ciborowski J
Ciesielski R
Cifarelli L
Cindolo F
Collaboration ZEUS
Contin A
Cooper-Sarkar AM
Coppola N
Corradi M
Corriveau F
Costa M
D'Agostini G
Dal Corso F
De Pasquale S
del Peso J
Dementiev RK
Derrick M
Devenish RCE
Dobur D
Dolgoshein BA
Dolinska G
Doyle AT
Drugakov V
Durkin LS
Dusini S
Eisenberg Y
Ermolov PF
Eskreys A
Fang S
Fazio S
Ferrando J
Ferrero MI
Figiel J
Forrest M
Foster B
Gach G
Galas A
Gallo E
Garfagnini A
Geiser A
Gialas I
Gladilin LK
Gladkov D
Glasman C
Goettlicher P
Gogota O
Golubkov YA
Grabowska-Bold I
Grebenyuk J
Gregor I
Grigorescu G
Grzelak G
Gueta O
Guzik M
Gwenlan C
Haas T
Hain W
Hamatsu R
Hart JC
Hartmann H
Hartner G
Hilger E
Hochman D
Hori R
Horton K
Huettmann A
Ibrahim ZA
Idris FM
Iga Y
Ingbir R
Ishitsuka M
Jakob H-P
Januschek F
Jones TW
Juengst M
Kadenko I
Kahle B
Kananov S
Kanno T
Karshon U
Karstens F
Katkov II
Kaur M
Kaur P
Keramidas A
Khein LA
Kim JY
Kisielewska D
Kitamura S
Klanner R
Klein U
Koetz U
Koffeman E
Kooijman P
Korol I
Korzhavina IA
Kotanski A
Kowalski H
Kuprash O
Kuze M
Lee A
Levchenko BB
Levy A
Libov V
Limentani S
Ling TY
Lisovyi M
Lobodzinska E
Loehr B
Lohmann W
Lohrmann E
Long KR
Longhin A
Lontkovskyi D
Lukina OY
Maeda J
Magill S
Makarenko I
Malka J
Mankel R
Margotti A
Marini G
Martin JF
Mastroberardino A
Mattingly MCK
Melzer-Pellmann I-A
Mergelmeyer S
Miglioranzi S
Monaco V
Montanari A
Morris JD
Mujkic K
Musgrave B
Nagano K
Namsoo T
Nania R
Nigro A
Ning Y
Nobe T
Noor U
Notz D
Nowak RJ
Nuncio-Quiroz AE
Oh BY
Okazaki N
Oliver K
Olkiewicz K
Onishchuk Y
Papageorgiu K
Parenti A
Paul E
Pawlak JM
Pawlik B
Pelfer PG
Pellegrino A
Perlanski W
Perrey H
Piotrzkowski K
Plucinski P
Pokrovskiy NS
Polini A
Proskuryakov AS
Przybycien M
Raval A
Reeder DD
Reisert B
Ren Z
Repond J
Ri YD
Robertson A
Roloff P
Rubinsky I
Ruspa M
Sacchi R
Salii A
Samson U
Sartorelli G
Savin AA
Saxon DH
Schioppa M
Schlenstedt S
Schleper P
Schmidke WB
Schneekloth U
Schoenberg V
Schoerner-Sadenius T
Schwartz J
Sciulli F
Shcheglova LM
Shehzadi R
Shimizu S
Singh I
Skillicorn IO
Slominski M
Smith WH
Sola V
Solano A
Son D
Sosnovtsev V
Spiridonov A
Stadie H
Stanco L
Stern A
Stewart TP
Stifutkin A
Stopa P
Suchkov S
Susinno G
Suszycki L
Sztuk-Dambietz J
Szuba D
Szuba J
Tapper AD
Tassi E
Terron J
Theedt T
Tiecke H
Tokushuku K
Tomalak O
Tomaszewska J
Tsurugai T
Turcato M
Tymieniecka T
Vazquez M
Verbytskyi A
Viazlo O
Vlasov NN
Volynets O
Walczak R
Whitmore JJ
Wiggers L
Wing M
Wlasenko M
Wolf G
Wolfe H
Wrona K
Yaguees-Molina AG
Yamada S
Yamazaki Y
Yoshida R
Youngman C
Zarnecki AF
Zawiejski L
Zenaiev O
Zeuner W
Zhautykov BO
Zhmak N
Zhou C
Zichichi A
Zolkapli Z
Zolko M
Zotkin DS
Publication venue
Publication date: 01/03/2012
Field of study

Scaled momentum distributions for the strange hadrons K0S and Λ/Λ¯ were measured in deep inelastic ep scattering with the ZEUS detector at HERA using an integrated luminosity of 330 pb−1. The evolution of these distributions with the photon virtuality, Q 2, was studied in the kinematic region 10 < Q 2 < 40000 GeV2 and 0.001 < x < 0.75, where x is the Bjorken scaling variable. Clear scaling violations are observed. Predictions based on different approaches to fragmentation were compared to the measurements. Leading-logarithm parton-shower Monte Carlo calculations interfaced to the Lund string fragmentation model describe the data reasonably well in the whole range measured. Next-to-leading-order QCD calculations based on fragmentation functions, FFs, extracted from e + e − data alone, fail to describe the measurements. The calculations based on FFs extracted from a global analysis including e + e −, ep and pp data give an improved description. The measurements presented in this paper have the potential to further constrain the FFs of quarks, anti-quarks and gluons yielding K0S and Λ/Λ¯ strange hadrons

UCL Discovery

Observation of Charge-Dependent Azimuthal Correlations in p-Pb Collisions and Its Implication for the Search for the Chiral Magnetic Effect

Author: Aarrestad T. K.
Abad D. R.
Abbaneo D.
Abbiendi G.
Abbrescia M.
Abdelalim A. A.
Abdullah Watw
Abdullin S.
Abdulsalam A.
Abercrombie D.
Abu Zeid S.
Ackert A.
Acosta D.
Acosta J. G.
Acosta M. V.
Adair A.
Adam W.
Adams J. R.
Adams M. R.
Adams T.
Adiguzel A.
Adzic P.
Afanasiev S.
Agapitos A.
Aggleton R.
Agram J. L.
Ahmad A.
Ahmad M.
Ahmad M.
Ahmed I.
Ahuja S.
Akbiyik M.
Akchurin N.
Akgun B.
Al-Bataineh A.
Albergo S.
Albert A.
Albrow M.
Alda W. L.
Alderweireldt S.
Aleksandrov A.
Alexander J.
Ali Mabm
Alimena J.
Allen B.
Almond J.
Alvarez J. D. R.
Alverson G.
Alves F. L.
Alves G. A.
Alyari M.
Amapane N.
Amin N.
Amsler C.
Anagnostou G.
Anampa K. H.
Anderson D.
Anderson I.
Andrea J.
Andreev V.
Andreev Y.
Andres I. S.
Andrews M. B.
Androsov K.
Anelli C.
Angioni G. L. P.
Antonelli L.
Antropov I.
Antunes J.
Antunovic Z.
Apanasevich L.
Apollinari G.
Apresyan A.
Apyan A.
Arcaro D.
Arcidiacono R.
Arenton M. W.
Argiro S.
Arndt T.
Arneodo M.
Asavapibhop B.
Asawatangtrakuldee C.
Asilar E.
Askew A.
Attikis A.
Aubin A.
Auffray E.
Autermann C.
Auzinger G.
Avdeeva E.
Avery P.
Avetisyan A.
Avila C.
Azarkin M.
Azhgirey I.
Aziz T.
Azzi P.
Azzolini V.
Azzurri P.
Baarmand M. M.
Baber M.
Bacchetta N.
Bachmair F.
Bachtis M.
Baden A.
Baffioni S.
Bagliesi G.
Bahinipati S.
Baillon P.
Bainbridge R.
Bakhshiansohi H.
Ball A. H.
Ball F.
Ban Y.
Banerjee S.
Banerjee S.
Bani L.
Bansal S.
Barbagli G.
Barberis E.
Barbieri R.
Bargassa P.
Baringer P.
Barker A.
Barnes V. E.
Barney D.
Baron O.
Barone L.
Barrera C. O.
Barria P.
Bartek R.
Barth C.
Bartok M.
Bartosik N.
Baskakov A.
Battilana C.
Baty A.
Bauerdick L. A. T.
Baur S.
Baus C.
Bayshev I.
Bean A.
Beauceron S.
Beaudette F.
Beck L.
Bedoya C. F.
Beernaert K.
Behera P. K.
Behnamian H.
Behnke O.
Behrens U.
Bein S.
Belforte S.
Beliy N.
Belknap D. A.
Bellan R.
Belloni A.
Beluffi C.
Belyaev A.
Belyaev A.
Benato L.
Bencze G.
Bendavid J.
Benelli G.
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Benussi L.
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Beranek S.
Beretvas A.
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del Arbol P. M. R.
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Tali B.
Talvitie J.
Tambe N.
Tan P.
Tan S. M.
Tao J.
Tao Z.
Tapper A.
Tarkovskii E.
Taroni S.
Tatar K.
Tatarinov A.
Tavernier S.
Tavolaro V. R.
Taylor D.
Taylor L.
Teles P. R.
Tenchini R.
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Terkulov A.
Teyssier D.
Thakur S.
Thapa K.
Thea A.
Theofilatos K.
Tholen H.
Thom J.
Thomas L.
Thomas S.
Thomassen P.
Thuer S.
Thyssen F.
Tiko A.
Tiras E.
Titov M.
Tkaczyk S.
Tlisov D.
Toda S.
Toldaiev O.
Tomalin I. R.
Tomei Trfp
Toms M.
Tonelli G.
Tonjes M. B.
Tonwar S. C.
Topaksu A. K.
Topkar A.
Topsis-Giotis I.
Torassa E.
Toriashvili T.
Toropin A.
Tosi M.
Tosi N.
Tosi S.
Traczyk P.
Tran N. V.
Treille D.
Trevisani N.
Tricomi A.
Triossi A.
Tripathi M.
Trocino D.
Trocsanyi Z. L.
Troendle D.
Troshin S.
Trovato M.
Tsai J. F.
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Tsiakkouri D.
Tsirou A.
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Turkewitz J.
Turner M.
Turner P.
Tuuva T.
Tuve C.
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Uchida K.
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Ulmer K. A.
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Uplegger L.
Usai E.
Uzunian A.
Vaandering E. W.
Vadruccio D.
Vai I.
Vaitkus J.
Valencia F. V.
Valuev V.
Van de Klundert M.
Van Doninck W.
Van Driessche W.
Van Haevermaet H.
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Veszpremi V.
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Veverka J.
Vidal R.
Vignali M. C.
Vila I.
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Virdee T.
Viret S.
Virto A. L.
Vischia P.
Vitulo P.
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Vlimant J. R.
Vogel H.
Volkov A.
Volobouev I.
Vormwald B.
Vorobiev I.
Vorobyev A.
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Voytishin N.
Vutova M.
Wagner S. R.
Wagner-Kuhr J.
Walczak M.
Walia G.
Walker M.
Wallny R.
Walsh R.
Waltenberger W.
Wang C.
Wang D.
Wang F.
Wang H.
Wang J.
Wang J.
Wang M.
Wang Q.
Wang R. J.
Wang S.
Wang T. W.
Wang Y.
Wang Z.
Wang Z.
Waqas M.
Wardle N.
Wasserbaech S.
Wayand S.
Wayne M.
Weber H.
Weber H. A.
Weber M.
Weber M.
Wei H.
Weiler T.
Weinberg M.
Welke C.
Wendland L.
Wertz S.
West C.
Wetzel J.
Whitbeck A.
Wickramage N.
Williams T.
Williamson S.
Wimpenny S.
Winer B. L.
Winn D.
Wissing C.
Wittich P.
Wohri H. K.
Wohrmann C.
Wolf M.
Wolf R.
Wolfe E.
Wood D.
Wood J.
Woodard A.
Woods N.
Wright D.
Wright J.
Wu Y.
Wu Z.
Wuerthwein F.
Wulsin H. W.
Wulz C. E.
Wyslouch B.
Xia F.
Xiao M.
Xie S.
Xie W.
Xin Y.
Xu Q.
Xu Z.
Yagil A.
Yalvac M.
Yang M.
Yang U. K.
Yang Y.
Yang Y. C.
Yates B. R.
Yazgan E.
Yelton J.
Yetkin E. A.
Yetkin T.
Yi K.
Yilmaz Y.
Yohay R.
Yonamine R.
Yoo H. D.
Yoo J.
You C.
Yu G. B.
Yu I.
Yu S. S.
Yumiceva F.
Yusli M. N.
Yzquierdo A. P. C.
Zabel J.
Zabi A.
Zaganidis N.
Zagozdzinska A.
Zakaria M.
Zalewski P.
Zanetti A.
Zanetti M.
Zarubin A.
Zeinali M.
Zenoni F.
Zenz S. C.
Zeuner W. D.
Zeyrek M.
Zghiche A.
Zhang F.
Zhang H.
Zhang J.
Zhao J.
Zhokin A.
Zhu R. Y.
Zhukov V.
Zhukova V.
Zientek M.
Zolkapli Z.
Zorbakir I. S.
Zorbilmez C.
Zotto P.
Zou D.
Zsigmond A. J.
Zucchetta A.
Zumerle G.
Zuranski A.
Zykunov V.
Publication venue
Publication date: 01/01/2016
Field of study

Peer reviewe

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Measurement of D+- and D0 production in deep inelastic scattering using a lifetime tag at HERA

Author: 16 ]
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3 ] Bindi
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3 ] Contin
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A[ 14
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A[ 33
A[ 36
A[ 39
A[ 4
A[ 4
A[ 44
A[ 7
Abdullah WATW[ 9 ]
Abramowicz
Abt I[ 32 ]
AD[ 2
Adamczyk L[ 12 ]
Adamus M[ 48 ]
Allfrey
AM[ 3
Antonelli
Antonioli P[ 3 ]
Antonov A[ 30 ]
Arneodo
Aushev V[ 24 ]
B[ 3
Bachynska O[ 24 ]
Bamberger A[ 18 ]
Barakbaev AN[ 23 ]
Barbagli G[ 16 ]
Bari G[ 3 ]
Barreiro F[ 27 ]
Bartsch D[ 5 ]
Behnke O[ 14 ]
Behrens U[ 14 ]
Bell
Bellagamba L[ 3 ]
Bellan
Bertolin A[ 35 ]
Bhadra S[ 51 ]
Blohm C[ 14 ]
Bold T[ 12 ]
Bonato A[ 14 ]
Boos EG[ 23 ]
Borodin M[ 24 ]
Borras K[ 14 ]
Boscherini D[ 3 ]
Bot D[ 14 ]
Boutle
Brock I[ 5 ]
Brook NH[ 52 ]
Brownson E[ 50 ]
Brugnera
Brummer N[ 34 ]
Bruni A[ 3 ]
Bruni G[ 3 ]
Brzozowska B[ 47 ]
Bussey PJ[ 19 ]
Butterworth
Bylsma B[ 34 ]
C[ 2
C[ 2
C[ 3
Caldwell A[ 32 ]
Capua
Carlin
Catterall CD[ 51 ]
Chekanov S[ 1 ]
Chwastowski J[ 11 ]
Ciborowski
Ciesielski R[ 14 ]
Cindolo F[ 3 ]
Cole
Cooper Sarkar
Coppola N[ 14 ]
Corradi M[ 3 ]
Corriveau F[ 28 ]
Costa
Cui Y[ 51 ]
D'Agostini
D[ 14
Dal Corso F[ 35 ]
de Favereau J[ 26 ]
DE PASQUALE Salvatore
del Peso J[ 27 ]
Dementiev RK[ 31 ]
Derrick M[ 1 ]
Devenish
Dobur D[ 18 ]
Dolgoshein BA[ 30 ]
Doyle AT[ 19 ]
Drugakov V[ 15 ]
Dunne W[ 19 ]
Durkin LS[ 34 ]
Dusini S[ 35 ]
E[ 33
E[ 7
Eisenberg Y[ 49 ]
Ermolov PF[ 31 ]
Eskreys A[ 11 ]
Fang S[ 14 ]
Fazio
Ferrando
Ferrero
Figiel J[ 11 ]
Forrest M[ 19 ]
Foster
Foudas
Fourletov S[ 46 ]
Fourletova J[ 14 ]
Fry
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Gallo E[ 16 ]
Garfagnini
Geiser A[ 14 ]
Gialas I[ 20 ]
Gladilin LK[ 31 ]
Gladkov D[ 30 ]
Glasman C[ 27 ]
Golubkov YA[ 31 ]
Gottlicher P[ 14 ]
Grabowska Bold I[ 12 ]
Grebenyuk J[ 14 ]
Gregor I[ 14 ]
Grigorescu
Grzelak G[ 47 ]
Gwenlan
H[ 33
H[ 40
Haas T[ 14 ]
Hain W[ 14 ]
Hall Wilton
Hamatsu R[ 43 ]
Hart
Hartmann H[ 5 ]
Hartner G[ 51 ]
Heath GP[ 52 ]
Hilger E[ 5 ]
Hochman D[ 49 ]
Holm U[ 21 ]
Hori R[ 42 ]
Horton
Huttmann A[ 14 ]
I[ 6
Iacobucci G[ 3 ]
Ibrahim ZA[ 9 ]
Idris F[ 9 ]
Iga Y[ 38 ]
Ingbir R[ 40 ]
J[ 14
J[ 3
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Jakob HP[ 5 ]
Januschek F[ 14 ]
JC[ 4
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JM[ 5
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Kagawa S[ 42 ]
Kahle B[ 14 ]
Kaji H[ 43 ]
Kamaluddin B[ 9 ]
Kananov S[ 40 ]
Karshon U[ 49 ]
Karstens F[ 18 ]
Katkov II[ 14 ]
Kaur
Kaur M[ 6 ]
Keramidas
Khein LA[ 31 ]
Kim JY[ 8 ]
Kisielewska D[ 12 ]
Kitamura S[ 43 ]
Klanner R[ 21 ]
Klein U[ 14 ]
Koffeman
Kollar D[ 32 ]
Kooijman
Korzhavina IA[ 31 ]
Kotanski A[ 13 ]
Kotz U[ 14 ]
Kowalski H[ 14 ]
Kozulia A[ 24 ]
KR[ 2
Kulinski P[ 47 ]
Kuze M[ 41 ]
Kuzmin VA[ 31 ]
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L[ 4
Labarga L[ 27 ]
Lee A[ 34 ]
Levchenko BB[ 31 ]
Levy A[ 40 ]
Libov V[ 24 ]
Limentani
Ling TY[ 34 ]
Lisovyi M[ 14 ]
Liu C[ 28 ]
Lobodzinska E[ 14 ]
Lohmann W[ 15 ]
Lohr B[ 14 ]
Lohrmann E[ 21 ]
Loizides
Long
Longhin A[ 35 ]
Lontkovskyi D[ 24 ]
Lukasik J[ 12 ]
Lukina OY[ 31 ]
Luzniak P[ 47 ]
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M[ 4
M[ 4
M[ 44
M[ 45
M[ 45
M[ 5
M[ 7
M[ 7
MA[ 3
Maeda J[ 41 ]
Magill S[ 1 ]
Makarenko I[ 24 ]
Malka J[ 47 ]
Mankel R[ 14 ]
Margotti A[ 3 ]
Marini
Martin JF[ 46 ]
Mastroberardino
Matsumoto T[ 22 ]
Mattingly MCK[ 2 ]
Melzer Pellmann IA[ 14 ]
Menary S[ 51 ]
MI[ 44
Miglioranzi S[ 14 ]
Molina AGY[ 14 ]
Monaco
Montanari A[ 14 ]
Morris JD[ 52 ]
MR[ 5
Musgrave B[ 1 ]
Nagano K[ 22 ]
Namsoo T[ 14 ]
Nania R[ 3 ]
Nicholass D[ 1 ]
Nigro
Ning Y[ 10 ]
Noor U[ 51 ]
Notz D[ 14 ]
Nowak RJ[ 47 ]
Nuncio Quiroz AE[ 5 ]
Oh BY[ 37 ]
Okazaki N[ 42 ]
Oliver
Olkiewicz K[ 11 ]
Ota O[ 43 ]
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Papageorgiu K[ 20 ]
Parenti A[ 14 ]
Paul E[ 5 ]
Pawlak JM[ 47 ]
Pawlik B[ 11 ]
PD[ 3
Pelfer
Pellegrino
Perlanski W[ 47 ]
Perrey H[ 21 ]
PG[ 17
Piotrzkowski K[ 26 ]
Plucinski P[ 48 ]
Pokrovskiy NS[ 23 ]
Polini A[ 3 ]
Proskuryakov AS[ 31 ]
Przybycie M[ 12 ]
R[ 3
R[ 36
R[ 36
R[ 44
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Raval A[ 37 ]
RCE[ 3
Reeder DD[ 50 ]
Reisert B[ 32 ]
Ren Z[ 10 ]
Repond J[ 1 ]
Ri YD[ 43 ]
Rinaldi L[ 14 ]
Robertson
Roloff P[ 14 ]
Ron E[ 27 ]
Rosin M[ 19 ]
Rubinsky I[ 14 ]
Ruspa
S[ 36
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S[ 4
S[ 7
Sacchi
Samson U[ 5 ]
Savin AA[ 50 ]
Saxon DH[ 19 ]
Schioppa
Schlenstedt S[ 15 ]
Schleper P[ 21 ]
Schmidke WB[ 32 ]
Schneekloth U[ 14 ]
Schonberg V[ 5 ]
Schorner Sadenius T[ 21 ]
Schwartz J[ 28 ]
Sciulli F[ 10 ]
Shcheglova LM[ 31 ]
Shehzadi R[ 5 ]
Shimizu S[ 42 ]
Singh
SK[ 5
Skillicorn IO[ 19 ]
Slominski W[ 13 ]
Smith WH[ 50 ]
Soares M[ 27 ]
Sola
Solano
Son D[ 25 ]
Sorokin I[ 24 ]
Sosnovtsev V[ 30 ]
Spiridonov
Stadie H[ 21 ]
Stanco L[ 35 ]
Standage J[ 51 ]
Stern A[ 40 ]
Stewart TP[ 46 ]
Stifutkin A[ 30 ]
Stopa P[ 11 ]
Suchkov S[ 30 ]
Susinno
Suszycki L[ 12 ]
Sutton
Sztuk J[ 21 ]
Szuba
Szuba
T[ 47
Tapper
Tassi
Tawara T[ 42 ]
Terron J[ 27 ]
Theedt T[ 14 ]
Tiecke
Tokushuku K[ 22 ]
Tsurugai T[ 29 ]
Turcato M[ 21 ]
TW[ 5
Tymieniecka
Ukleja A[ 48 ]
Ukleja J[ 14 ]
Uribe Estrada C[ 27 ]
V[ 44
V[ 44
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Verbytskyi A[ 24 ]
Vlasov NN[ 18 ]
Volynets O[ 24 ]
Walczak
Walsh R[ 28 ]
Whitmore JJ[ 37 ]
Whyte J.
Wiggers
Wing
Wlasenko M[ 5 ]
Wolf G[ 14 ]
Wolfe H[ 50 ]
Wrona K[ 14 ]
Yamada S[ 22 ]
Yamazaki Y[ 22 ]
Yoshida R[ 1 ]
Youngman C[ 14 ]
Zambrana M[ 27 ]
Zarnecki AF[ 47 ]
Zawiejski L[ 11 ]
Zeuner W[ 14 ]
Zhautykov BO[ 23 ]
Zhou C[ 28 ]
Zotkin DS[ 31 ]
Publication venue
Publication date: 01/01/2008
Field of study

The production of D-+/-- and D-0-mesons has been measured with the ZEUS detector at HERA using an integrated luminosity of 133.6 pb(-1). The measurements cover the kinematic range 5 < Q(2) < 1000 GeV2, 0.02 < y < 0.7, 1.5 < p(T)(D) < 15 GeV and |eta(D)| < 1.6. Combinatorial background to the D-meson signals is reduced by using the ZEUS microvertex detector to reconstruct displaced secondary vertices. Production cross sections are compared with the predictions of next-to-leading-order QCD, which is found to describe the data well. Measurements are extrapolated to the full kinematic phase space in order to obtain the open-charm contribution, F-2(c (c) over bar), to the proton structure function, F-2

EDP Sciences OAI-PMH repository (1.2.0)

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International Migration, Integration and Social Cohesion online publications

UvA-DARE

Archivio istituzionale della ricerca - Università di Padova

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Andrews University

Archivio della Ricerca - Università di Salerno

Study of B Meson Production in p plus Pb Collisions at root s(NN)=5.02 TeV Using Exclusive Hadronic Decays

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Publication venue
Publication date: 01/01/2015
Field of study

Peer reviewe

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Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}

Author: Aarrestad TK
Abbaneo D
Abbiendi G
Abbrescia M
Abdalla H
Abdelalim AA
Abdullah WATW
Abdullin S
Abdulsalam A
Abercrombie D
Abu Zeid S
Ackert A
Acosta D
Acosta JG
Adam W
Adams MR
Adams T
Adzic P
Afanasiev S
Agapitos A
Agaras MN
Aggleton R
Agram J-L
Ahmad A
Ahmad M
Ahmed I
Ahuja S
Akbiyik M
Akchurin N
Akgun B
Al-bataineh A
Albajar C
Albergo S
Albert A
Albrow M
Alcaraz Maestre J
Aleksandrov A
Alexander J
Alhusseini M
Ali MABM
Alimena J
Allen B
Almond J
Alvarez Fernandez A
Alvarez JDR
Alverson G
Alves FL
Alves GA
Alyari M
Amapane N
Ambrogi F
Amendola C
Amin N
Amsler C
Anagnostou G
Anampa KH
Anderson D
Andrea J
Andreev V
Andreev Y
Andrews MB
Androsov K
Angioni GLP
Antonelli L
Antropov I
Antunes De Oliveira AC
Antunovic Z
Apanasevich L
Apollinari G
Apresyan A
Apyan A
Araujo M
Arcaro D
Arcidiacono R
Arenton MW
Argiro S
Arndt T
Arneodo M
Asavapibhop B
Asawatangtrakuldee C
Asghar M
Asilar E
Askew A
Atakisi IO
Ather MW
Attikis A
Auffray E
Aushev T
Autermann C
Auzinger G
Avdeeva E
Avery P
Avila C
Ayala E
Azarkin M
Azhgirey I
Aziz T
Azzi P
Azzolini V
Azzurri P
Baarmand MM
Babaev A
Babounikau I
Bacchetta N
Bachiller I
Bachtis M
Backhaus M
Baden A
Bagliesi G
Bahinipati S
Baidali S
Baillon P
Bainbridge R
Bakhshiansohi H
Ball AH
Ball F
Ban Y
Band R
Banerjee S
Bani L
Bansal S
Barbagli G
Barberis E
Bargassa P
Baringer P
Barker A
Barnes VE
Barney D
Barnyakov A
Baron O
Barone L
Barria P
Barrio Luna M
Bartek R
Barth C
Bartok M
Bartosik N
Baselga M
Baskakov A
Bat A
Battilana C
Baty A
Bauer G
Bauerdick LAT
Baur S
Bayshev I
Bean A
Beauceron S
Beaudette F
Becerra DAS
Beernaert K
Beghin D
Behera PK
Behnke O
Behrens U
Bein S
Beirao Da Cruz E Silva C
Belchior Batista Das Chagas E
Belforte S
Bell KW
Bellan R
Belloni A
Belyaev A
Benaglia A
Benato L
Bencze G
Bendavid J
Benecke A
Benelli G
Beni N
Benitez JF
Benussi L
Benvenuti AC
Beretvas A
Bergauer T
Berger P
Beri SB
Bernardes CA
Bernet C
Berry D
Berryhill J
Bertsche D
Besancon M
Beschi A
Betts RR
Bhandari R
Bhardwaj A
Bhardwaj R
Bharti M
Bhat MA
Bhat PC
Bhatnagar V
Bhattacharya R
Bhattacharya S
Bhawandeep U
Bheesette S
Bhopatkar V
Bhowmik D
Bhowmik S
Bi R
Bialkowska H
Bian JG
Bianchini L
Bianco M
Bianco S
Biasini M
Biino C
Bilei GM
Bilin B
Bilki B
Bin Anuar AA
Bisello D
Bitioukov S
Blanco JM
Blekman F
Blinov V
Blobel V
Bloch D
Bloch P
Bloom K
Bluj M
Blumenfeld B
Boccali T
Bocci A
Bodek A
Boimska B
Boletti A
Bonacorsi D
Bondu O
Boos E
Boran F
Boren S
Borg J
Borgonovi L
Bornheim A
Borras K
Borrello L
Bortignon P
Bose T
Botta C
Botta V
Boudoul G
Bouhali O
Bourilkov D
Bouvier E
Bowen J
Bragagnolo A
Braghieri A
Braibant-Giacomelli S
Brainerd C
Brandstetter J
Brandt S
Branson JG
Bravo C
Breedon R
Breeze S
Brew C
Brigljevic V
Brinkerhoff A
Brivio F
Brochero Cifuentes JA
Brochet S
Brodski M
Brom J-M
Brondolin E
Brooke JJ
Brown RM
Brun H
Bruno G
Brzhechko D
Bucci R
Buccilli A
Buchanan J
Buchmuller O
Bueghly J
Bundock A
Bunichev V
Bunin P
Bunkowski K
Buontempo S
Burkett K
Burns D
Burt K
Busson P
Busza W
Butler JN
Butler PH
Butz E
Bylinkin A
Bylsma B
Byszuk A
Cabrera A
Cabrillo IJ
Cadamuro L
Caillol C
Cakir A
Calabria C
Calderon A
Cali IA
Call K
Calligaris L
Caminada L
Campagnari C
Campanini R
Campbell A
Camporesi T
Candelise V
Canelli MF
Canepa A
Cankocak K
Capiluppi P
Cappati A
Caputo C
Carlin R
Carlsmith D
Carnes A
Carrera Jarrin E
Carrillo Montoya CA
Carrillo Moreno S
Cartiglia N
Carvalho W
Casarsa M
Caspart R
Castaldi R
Castaneda Hernandez A
Castilla-Valdez H
Castle J
Castro A
Cavallari F
Cavallo FR
Cavallo N
Cavanaugh R
Ceballos GG
Cecchi C
Celik A
Cenna F
Cepeda M
Cerati GB
Cerci S
Cerminara G
Cerrada M
Chabert EC
Chadeeva M
Chang P
Chanon N
Chao Y
Chaparro Sierra LF
Chapon E
Charaf O
Charlot C
Chatterjee K
Chatterjee RM
Chatterjee S
Chauhan S
Chaves J
Chawla R
Chazin Quero B
Checchia P
Chekhovsky V
Chen G
Chen GM
Chen HS
Chen KF
Chen M
Chen PH
Chen X
Chen Y
Chen Z
Chenarani S
Cheng T
Cheng Y
Cherepanov V
Chernyavskaya N
Chertok M
Cheung HWK
Chhibra SS
Chierici R
Chinellato J
Chlebana F
Cho S
Choi S
Choi Y
Chou JP
Choudhary BC
Choudhury S
Chowdhury SR
Chu J
Chudasama R
Chwalek T
Ciangottini D
Cieri D
Ciocca C
Ciocci MA
Cipriani M
Ciriolo V
Cirkovic P
Citron M
Cittolin S
Ciulli V
Civinini C
Claes DR
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Publication venue: 'Elsevier BV'
Publication date: 10/09/2019
Field of study

The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons

UCL Discovery

Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV

Author: Aarrestad TK
Abbaneo D
Abbiendi G
Abbrescia M
Abdalla H
Abdullah WATW
Abdullin S
Abdulsalam A
Abercrombie D
Abu Zeid S
Acharya H
Ackert A
Acosta D
Acosta JG
Adam W
Adams MR
Adams T
Adzic P
Afanasiev S
Agapitos A
Agaras MN
Aggleton R
Agram J-L
Ahmad A
Ahmad M
Ahmad M
Ahuja S
Akbiyik M
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Alcaraz Maestre J
Aleksandrov A
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Ali MABM
Alimena J
Allen B
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Alvarez Fernandez A
Alverson G
Alves FL
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Alyari M
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Ambrogi F
Amendola C
Amin N
Amsler C
Anagnostou G
Anampa KH
Anderson D
Andrea J
Andreev V
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Andrews MB
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Angioni GLP
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Atakisi IO
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Azzolini V
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Baarmand MM
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Becerra DAS
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Belchior Batista Das Chagas E
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de Monchenault GH
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Yu SS
Yuan L
Yumiceva F
Yusli MN
Zabi A
Zaganidis N
Zahid S
Zaleski S
Zalewski P
Zanetti A
Zanetti M
Zarubin A
Zarucki M
Zeinali M
Zenaiev O
Zenz SC
Zeuner WD
Zeyrek M
Zghiche A
Zhang A
Zhang F
Zhang H
Zhang J
Zhang S
Zhang Z
Zhao J
Zhokin A
Zhu DH
Zhu RY
Zientek M
Zobec J
Zoi I
Zolkapli Z
Zorbakir IS
Zorbilmez C
Zotto P
Zou D
Zucchetta A
Zumerle G
Zuo X
Zuolo D
Publication venue: 'Springer Fachmedien Wiesbaden GmbH'
Publication date: 29/04/2019
Field of study

A measurement of the top quark–antiquark pair production cross section σtt¯ in proton–proton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fb−1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± μ ∓, μ+μ−, e+e−) are selected and the cross section is measured from a likelihood fit. For a top quark mass parameter in the simulation of mMCt=172.5GeV the fit yields a measured cross section σtt¯=803±2(stat)±25(syst)±20(lumi)pb, in agreement with the expectation from the standard model calculation at next-to-next-to-leading order. A simultaneous fit of the cross section and the top quark mass parameter in the POWHEG simulation is performed. The measured value of mMCt=172.33±0.14(stat)+0.66−0.72(syst)GeV is in good agreement with previous measurements. The resulting cross section is used, together with the theoretical prediction, to determine the top quark mass and to extract a value of the strong coupling constant with different sets of parton distribution functions

UCL Discovery

Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV

Author: Aarrestad TK
Abbaneo D
Abbiendi G
Abbrescia M
Abdullah WATW
Abdullin S
Abercrombie D
Acharya H
Acosta D
Acosta JG
Adam W
Adams E
Adams MR
Adams T
Adloff C
Adzic P
Adán DP
Afanasiev S
Agapitos A
Agarwal G
Aggleton R
Agram J-L
Aguilar-Benitez M
Ahmad A
Ahmad M
Ahmad WH
Ahmed A
Ahuja S
Aime' C
Akchurin N
Akgun B
Akpinar A
Albajar C
Albergo S
Albert A
Albrow M
Aleksandrov A
Alexander J
Alhusseini M
Alimena J
Alison J
Allen B
Almond J
Alonso AG
Alvarez JDR
Alverson G
Alves GA
Aly R
Alyari M
Amapane N
Amaral SMSD
Amendola C
Amin N
Amram O
Amsler C
Anagnostou G
Anampa KH
Anderson D
Andrea J
Andreev V
Andreev Y
Andrews MB
Androsov K
Angioni GLP
Antchev G
Antunovic Z
Anuar AAB
Apanasevich L
Apollinari G
Appelt E
Apresyan A
Apyan A
Araujo M
Arbelaez NV
Arbol PMRD
Arcaro D
Arcidiacono R
Arenton MW
Argiro S
Arneodo M
Aruta C
Asavapibhop B
Asawatangtrakuldee C
Asenov P
Asghar MI
Asilar E
Askew A
Asmuss P
Atakisi IO
Atanasov I
Ather MW
Attikis A
Auffray E
Aushev T
Auzinger G
Avati V
Avery P
Avila C
Awan MIM
Ayala E
Ayala G
Azarkin M
Azhgirey I
Aziz T
Azzi P
Azzurri P
Baarmand MM
Babaev A
Babounikau I
Bacchetta N
Bachiller I
Bachtis M
Backhaus M
Baden A
Baechler J
Bagliesi G
Bahinipati S
Baillon P
Bainbridge R
Bakas G
Bakhshiansohi H
Ball AH
Ban Y
Band R
Bandyopadhyay H
Banerjee S
Banerjee S
Banos LIE
Bansal S
Barbagli G
Barberis E
Bargassa P
Baringer P
Barnes VE
Barney D
Baron O
Barrera CB
Barrera CO
Bartek R
Bartosik N
Bartók M
Bastos D
Battilana C
Baty A
Bauerdick LAT
Baur S
Baxter S
Bayshev I
Bean A
Beauceron S
Beaudette F
Becerra DAS
Bechtel J
Bedoya CF
Beghin D
Behera PK
Behera SC
Behnke O
Bein S
Belforte S
Bell KW
Bellan R
Belloni A
Bellora A
Belyaev A
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Benaglia A
Benato L
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Benecke A
Benelli G
Beni N
Benitez JF
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Beretvas A
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Beri SB
Bernardes CA
Bernet C
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Berryhill J
Bertacchi V
Besancon M
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Bhardwaj A
Bharti M
Bhat MA
Bhat PC
Bhatnagar V
Bhattacharya R
Bhattacharya S
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Bhyun JH
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Bianco M
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Biasini M
Bihan A-CL
Biino C
Bilei GM
Bilin B
Bindhu VKMN
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Bloch D
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Bloom K
Bluj M
Blumenfeld B
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Bocci A
Bodek A
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Bonomally S
Boos E
Boran F
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Bornheim A
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Brown RM
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Brzhechko D
Brücken E
Bucci R
Buccilli A
Buchanan J
Buchmuller O
Bueghly J
Bundock A
Bunichev V
Bunin P
Bunkowski K
Buontempo S
Burgo RD
Burkett K
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Butler JN
Butler PH
Butz E
Bylinkin A
Bylsma B
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Caballero IG
Cabrera A
Cabrillo IJ
Cadamuro L
Caillol C
Cakir A
Calandri A
Calderon A
Cali IA
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Camen C
Caminada L
Campagnari C
Campanini R
Campbell A
Campderros JD
Camporesi T
Candelise V
Canelli MF
Canepa A
Cankocak K
Capiluppi P
Cappati A
Caputo C
Caraway B
Cardini A
Cardwell B
Carle A
Carlin R
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Castaldi R
Castilla-Valdez H
Castro A
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Cavallo FR
Cavallo N
Cavanaugh R
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Ceballos GG
Ceccarelli R
Cepaitis V
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Chahal GS
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Chatterjee RM
Chatterjee S
Chauhan S
Chauhan S
Chawla R
Checchia P
Chekhovsky V
Chen C
Chen GM
Chen HS
Chen KF
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Chen PH
Chen X
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Chen Z
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Cherepanov V
Chernyavskaya N
Chertok M
Cheung HWK
Chhibra SS
Chiarito B
Chinellato J
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Chwalek T
Ciangottini D
Cifuentes JAB
Ciocci MA
Cipriani M
Ciriolo V
Cirkovic P
Citron M
Cittolin S
Ciulli V
Civinini C
Claes DR
Clare R
Clement E
Clerbaux B
CMS Collaboration
Cockerill DJA
Coelho E
Colaleo A
Cole JE
Colino N
Collard C
Colling D
Cometti S
Connor P
Contardo D
Conway J
Conway R
Cooper SI
Cooperstein S
Corcodilos L
Cornelis T
Cortezon EP
Cosby C
Cossutti F
Costa M
Costa S
Coubez X
Couderc F
Cousins R
Covarelli R
Cox B
Cox PT
Cranshaw DJ
Creanza D
Cremonesi M
Cristella L
Croce DD
Cruz SS
Csanad M
Csorgo T
Cuevas J
Cuffiani M
Cumalat JP
Cummings G
Cussans D
Cutts D
Czellar S
D'Alessandro R
D'Alfonso M
D'Enterria D
D'Hondt J
Da Costa EM
Da Rold A
Da Silva De Araujo FT
Da Silveira GG
Dabrowski A
Daci N
Dalchenko M
Dallavalle GM
Damarseckin S
Damgov J
Damiani DD
Danilov M
Danilov V
Daponte V
Darwish MR
Das P
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Dasgupta A
Dash D
Daskalakis G
Dasu S
Datta A
Dauncey P
David A
David P
Davies G
Davignon O
De Barbaro P
De Boer W
De Bruyn I
De Cassagnac RG
De Castro Manzano P
De Clercq J
De Cosa A
De Fatis TT
De Filippis N
De Guio F
De Iorio A
De Jesus Damiao D
De Klundert MV
De La Barca Sanchez MC
De La Cruz B
De La Cruz-Burelo E
De Lentdecker G
De Leo K
De Monchenault GH
De Oliveira ACA
De Palma M
De Roeck A
De Souza SF
De Trocóniz JF
De Wit A
De Wolf EA
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Defranchis MM
Deile M
Dejardin M
Delaere C
Delannoy AG
Delcourt M
Delgado A
Delgado MAS
Dell'Orso R
Demaria N
Demina R
Demiragli Z
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Dewanjee RK
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Dimitrov A
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Dinardo ME
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Dissertori G
Dittmann J
Dittmar M
Dittmer S
Dobson M
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Publication venue
Publication date: 01/01/2018
Field of study

A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe

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Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV

Author: Aarrestad TK
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Abbiendi G
Abbrescia M
Abdullah WATW
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Abercrombie D
Abu Zeid S
Ackert A
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Pflitsch SK
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Pilot J
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Pitters FM
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Planer M
Pol ME
Polatoz A
Polikarpov S
Pompili A
Pook T
Pooth O
Popov A
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Postiau N
Potenza R
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Poyraz D
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Prado Da Silva WL
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Qiu H
Qu H
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Rad N
Radburn-Smith BC
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Rakness G
Ramirez-Garcia M
Ramirez-Sanchez G
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Salazar Ibarguen HA
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Sanchez Rosas LJ
Sanchez MCDLB
Sanchez-Hernandez A
Sandeep K
Sanders S
Sani M
Santanastasio F
Santocchia A
Santoro A
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Sarica U
Sarkar S
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Sauvan JB
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Savoy-Navarro A
Savrin V
Saxena P
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Publication venue: 'Springer Fachmedien Wiesbaden GmbH'
Publication date: 01/01/2019
Field of study

A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of 36 fb^{-1}. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale Λ. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter Λ_{T} below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to Λ_{T} below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states

UCL Discovery